We study a generalized derivative nonlinear Schrödinger equation on a bounded interval under homogeneous Dirichlet boundary conditions. Starting from the local $ H^2 $ well-posedness theory, we derive a quantitative $ H^2 $ energy inequality in physical space. The estimate yields a genuine continuation criterion at a finite endpoint, divergence of the controlling $ W^{1, \infty} $ time integral whenever the maximal time is finite, the $ H^2 $ blow-up alternative, a quantitative lower blow-up rate, and an explicit lower bound for the lifespan in terms of the initial $ H^2 $ norm. The key mechanism is a derivative-loss cancellation in the highest-order transport term. Thus, the local existence theory is supplemented by explicit maximal-time information and computable growth scales.
Citation: Senyue Luo, Meilan Qiu, Zhiming Tan. Maximal-time criteria for a generalized derivative nonlinear Schrödinger equation[J]. AIMS Mathematics, 2026, 11(8): 27448-27467. doi: 10.3934/math.20261098
We study a generalized derivative nonlinear Schrödinger equation on a bounded interval under homogeneous Dirichlet boundary conditions. Starting from the local $ H^2 $ well-posedness theory, we derive a quantitative $ H^2 $ energy inequality in physical space. The estimate yields a genuine continuation criterion at a finite endpoint, divergence of the controlling $ W^{1, \infty} $ time integral whenever the maximal time is finite, the $ H^2 $ blow-up alternative, a quantitative lower blow-up rate, and an explicit lower bound for the lifespan in terms of the initial $ H^2 $ norm. The key mechanism is a derivative-loss cancellation in the highest-order transport term. Thus, the local existence theory is supplemented by explicit maximal-time information and computable growth scales.
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